TWI239434B - Method and apparatus of detecting aberrations with an optical system, lens aberration monitor and device manufacturing method - Google Patents
Method and apparatus of detecting aberrations with an optical system, lens aberration monitor and device manufacturing method Download PDFInfo
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- TWI239434B TWI239434B TW090128361A TW90128361A TWI239434B TW I239434 B TWI239434 B TW I239434B TW 090128361 A TW090128361 A TW 090128361A TW 90128361 A TW90128361 A TW 90128361A TW I239434 B TWI239434 B TW I239434B
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/20—Exposure; Apparatus therefor
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70483—Information management; Active and passive control; Testing; Wafer monitoring, e.g. pattern monitoring
- G03F7/70591—Testing optical components
- G03F7/706—Aberration measurement
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- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
- Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
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- Preparing Plates And Mask In Photomechanical Process (AREA)
Abstract
Description
1239434 A7 B71239434 A7 B7
本發明係關於偵測與使用於微影投影裝置中之光學系統( 例如投影系統以及/或是照射系統)關聯之像差,並且更特別 的是關於可以在使用此類裝置之半導體(以及其它)製造期間 用以監視该光學系統效能的像差監視結構的設計,配置 (layout)及應用。微影投影裝置通常包括: -一種用以供應照射投影光束之照射系統;The present invention relates to the detection of aberrations associated with optical systems (such as projection systems and / or illumination systems) used in lithographic projection devices, and more particularly relates to semiconductors (and other ) Design, layout, and application of aberration monitoring structures used to monitor the effectiveness of the optical system during manufacturing. The lithographic projection apparatus usually comprises:-an irradiation system for supplying an irradiation projection beam;
-一種用以支撐圖案構件之支撐結構,該圖案構件係根據 所要的圖案產生該投影光束之圖案; -一種用以承托基板之基板平台;以及 _ 一種用以將圖案光束投影至該基板目標位置之投影系統。 訂-A support structure for supporting a pattern member, the pattern member generating a pattern of the projection beam according to a desired pattern;-a substrate platform for supporting a substrate; and _ a method for projecting a pattern beam onto the substrate target Position projection system. Order
在此所使用的專有名詞”圖案構件,,大體上應該解釋為可用 於提供入射光束及圖案橫斷面之構件,符合想要在基板之 目標位置處創造之圖案;本文中亦使用到專有名詞,,光閥 (light valve)”。一般而言,該圖案相當於產生在目標處的元 件内之特殊功能層.,例如積體電路或其它元件(參見如下)。 此類圖案構件包括: -一種光罩。光罩的概念係微影中所熟知的,並且其包括 類似二元的,相位移交替,及衰減式相位移的光罩型式 ,以及各種的混成光罩型式。此類光束中光罩的擺放會 根據光罩上之圖案對於照射在該光罩上的光線產生選擇 性的傳送(如果是傳送光罩的話)或反射(如果是反射光罩 的話)。就光罩而言,通常該支撐結構會是一光罩平台, 其確保該光罩可以支撐在該入射光束所希望之位置上, -4- 本紙張纽如中國國家標準(CNS) A4規格(21〇 X 297公董) A7 B7 1239434 五、發明説明(2 並且如果需要的話,可以移動相對於該光束移動。 --種可程式鏡陣列。此類裝置之實例係一具有黏著伸縮 (ViSC〇elaStiC)控制層及反射表面之矩陣可定址表面 (matnx-addressable surface)。此類裝置的基本理係(舉例 來說)該反射表面之定址區會將入射光反射成繞射光,而 未定址區則會將入射光反射成非繞射光。利用適當的過 滤,該非繞射光會從該反射光束被過料,只留下繞射 光;在此万式下,該光束便會根據矩陣可定址表面之定 址圖案形成圖案。所需要之矩料址可以利用適當的電 子構件執行。有關此類鏡陣列之更多資訊可以從,舉例 來說,從美國專利us 5,296,89uUS mu93中取得, 此處予以參考引用。至於可程式鏡陣列,該支撐結構可 以具體化成一框架(frame)或平台,舉例來說,其可依 要固定或移動。 -一種可程式LCD陣列。此類結構之實例如美國專利1;3 5,229,872中所提出的,此處予以參考引用。如上所述, 在此例子中之支撐結構可以具體化成一框架或平台,舉 例來說,可依需要固定或移動。 為了簡單化,在後面的内容中,在某些位置,會特別針對 使用光罩及光罩平台的實例作說明;然而在這些例子中所 討論的原理都可以在上面提出的圖案構件内容中發現。 微影投影裝置可以使用於,舉例來說,積體電路的製造。 在此類實例中,該圖案構件可以產生與IC之個別層相符之 電路圖案,並且此圖案可以映射在已塗上一層感光材料(於 -5- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)The term “pattern component” used here should be interpreted as a component that can be used to provide the incident light beam and the cross-section of the pattern. It conforms to the pattern that you want to create at the target position of the substrate. There is a noun, light valve ". In general, the pattern corresponds to a special functional layer within the component produced at the target, such as an integrated circuit or other component (see below). Such pattern members include:-A photomask. The concept of photomask is well-known in lithography, and it includes two types of photomasks like binary, alternating phase shift, and attenuation phase shift, as well as various mixed photomask types. The placement of the reticle in such beams will selectively transmit (if a reticle) or reflect (if a reflective reticle) the light shining on the reticle according to the pattern on the reticle. As far as the photomask is concerned, the supporting structure is usually a photomask platform, which ensures that the photomask can be supported at the desired position of the incident light beam. -4- This paper is like the Chinese National Standard (CNS) A4 specification ( 21〇X 297 public director) A7 B7 1239434 V. Description of the invention (2 and if necessary, it can be moved relative to the beam.-A programmable mirror array. An example of such a device is an adhesive telescopic (ViSC〇 elaStiC) matnx-addressable surface of the control layer and reflective surface. The basic principle of such devices is (for example) the addressing area of the reflective surface will reflect incident light into diffracted light, while the unaddressed area The incident light will be reflected as non-diffractive light. With proper filtering, the non-diffractive light will be passed through the reflected beam, leaving only the diffracted light; in this mode, the beam will be addressed according to the addressable surface of the matrix The pattern forms a pattern. The required momentary address can be performed using appropriate electronic components. More information about such mirror arrays can be taken from, for example, US patent US 5,296,89uUS mu93 Here, as for the programmable mirror array, the support structure can be embodied as a frame or platform, for example, it can be fixed or moved as required.-A programmable LCD array. Such a structure Examples are proposed in U.S. Patent 1; 3, 5,229,872, which is incorporated herein by reference. As mentioned above, the support structure in this example can be embodied as a framework or platform, for example, can be fixed or For the sake of simplicity, in the following content, in some positions, the examples of using the mask and the mask platform will be specifically explained; however, the principles discussed in these examples can be based on the content of the pattern members proposed above. Found in the lithographic projection device can be used, for example, in the manufacture of integrated circuits. In such examples, the pattern member can generate a circuit pattern that matches the individual layers of the IC, and the pattern can be mapped on the painted Previous layer of photosensitive material (at -5- this paper size applies to China National Standard (CNS) A4 specifications (210 X 297 mm)
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1239434 A7 B7 五、發明説明(3 ) 蝕劑)之基板(矽晶圓)上的目標位置(例如包括一個或多個晶 粒)。一般而言,單晶圓會包含鄰近目標部分,其係透過投 射系統一次照射一個,的整個網路。在目前的裝置中,利 用光罩平台上之光罩進行圖案處理,可以區分不同的機器 型式。在其中一種微影投影裝置中,每一目標位置係利用 將正個光罩圖案曝光在目標位置作進行照射,·此類裝置一 般稱之為晶圓步進器(wafer stepper)。在替代的裝置中一_一 般%足為步進-掃描(step_and-scan)裝置-每一目標部分的照 射係利用在投影光束下以預定的參考方向("掃描"方向)漸 進式地掃描並且同時以與該方向平行或反方向掃描該基板 平台;因為,通常,該投影系統具有一放大係數撾(通常 < 1 ),所以掃描該基板平台的速度V會是掃描該光罩平台速 度的Μ倍。關於此處所述之微影裝置的更多資訊可以從us 6,046,792中得知’此處予以參考引用。 在此類利用微影投影裝置之製造過程中,在光罩(或其它 圖案構件)中之圖案係映射到至少部份被感光材料(抗蝕劑) 覆蓋之基板上。在此映射步驟之前,該基板會進行各種程 序,例如上底漆(pnming),抗蝕劑塗抹以及軟烘烤(S〇R bake)。在曝光之後,該基板會進行其它的程序,例如後曝 光洪烤(p〇St-exP〇sure bake,PEB),顯影,硬烘烤(hard bake)以及映射特徵測量/檢查。此程序係作為裝置',例如積 體電路(1C),之個別層圖案處理之基礎。接著此類圖案^ 理過的層會經過各種程序例如蝕刻,離子植入(摻雜),金屬 化,氧化,化學-機械研磨等,全部程序都是想要完成一個 -6 - 1239434 A7 B7 五、發明説明(4 ) 別層。如果需要數個層的話,那麼該整個程序,或其變化 ,便必須對每一新層重覆一遍。最後,便會在該基板(晶圓) 上呈現出一裝置陣列。接著便會利用類似切割(dicing)或鋸 開(sawing)的技術將該些裝置互相分離,因此個別裝置可以 安裝在一載具(carrier)上,連接至針腳等。關於此類程序之 進一步資訊可以從Peter van Zant所著之’’Microchip Fabrication : A Practical Guide to Semiconductor Processing”,第三版,由 McGraw Hill Publishing Co.於 1997 出版ISBN 0-07-067250-4—書中取得。 為了簡單起見,此後該投影系統將稱之為n透鏡π ;然而, 該專有名詞大體上應被解釋為包含各種投影系統之型式, 包括,舉例來說,折射光學系統,反射光學系統,以及全 折光(catadioptric)系統。該照射系統還包括根據任何一種設 計型式操作的元件,用以導向,定形或控制該照射投影光 束,並且此類元件在下面亦稱之為’’透鏡”。此外,微影裝 置也可以是具有兩個或多個基板平台(以及/或是兩個或更多 個光罩平台)之型式。在此類’’多重階段”裝置中該額外平台 可以同時使用,在一個或多個平台上進行準備步驟,而將 一個或多個其它平台作為曝光使用。舉例來說,雙階段微 影裝置在US 5,969,441以及W0 98/40791中有所說明,此處 予以參考引用。 目前的I C製造狀況需要微影程序以提供給圖案特徵線寬 度接近曝光波長的二分之一。以150nm的裝置來說,通常會 選擇KrF準分子雷射(excimer laser)(DUV ; 248nm)作為曝光 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 1239434 A7 B7 五、發明説明(5 ) 源。近來之研究及發展已經可以在130nm的裝置中利用KrF 準分子雷射。這可以利用多重解晰強化技術(RET)達成此目 的,例如衰減式相位偏移光罩(attPSM)以及離軸(off-axis) 照明(ΟΑΙ),結合光學鄰近修正(optical proximity correction,OPC)技術。可以利用上述技術之替代技術使用 較短的曝光波長,例如具有193 nm波長之ArF準分子雷射, 或使用具有超高數字孔徑(NA)之透鏡,例如NA=0.8或更大 。然而,該些替代技術皆需要在新裝置中投入龐大的資本 支出,並且如果可行的話一般都會希望延遲此類支出。因 此,整合元件製造商一般都希望可以在切換成接替設備之 前從現存的DUV系統中得到最大的效益。 不管在該製造程序中所使用的準分子雷射,製造具有 150nm或更小之關键尺寸之裝置需要使用於製造過程中的 近-繞射-限制(near-diffraction-limited)透鏡沒有像差。如所 熟知的,像差可以由各種不同來源造成,例如缺陷透鏡, 或老化雷射其發出的光束頻率已經與希望值產生偏移。因 此,希望檢查在裝置之前可以透鏡效能(換言之驗證該透鏡) ,並且隨後於使用期間(例如在I C製造過程中)監視該透鏡 效能。 在製造透鏡過程中,該透鏡效能可以以干涉方式 (interferometrically)進行完全測試。通常,會先在工廒驗證 該透鏡,然後在實地首次安裝時再次驗證。一種常用以驗 證透鏡的方法係印刷晶圓接著測量最小特徵寬度的尺寸, 或該關键尺寸(Critical Dimension,CD)。在驗證過程中,會 -8- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 1239434 A7 B7 五、發明説明(6 ) 測量”垂直”及”水平”特徵(換言之在該基板平面上兩個正交 方向延伸,例如沿著X及Y軸,的特徵)。在部分實例中, 也會測量4 5度特徵之CD。為了檢查透鏡之效能,必須在整 個曝光中進行充分的CD測量次數。接著會分析CD測量之 結果以判斷透鏡之效能是否可以接受。 雖然CD測量方法提供一種評估透鏡效能之方法,但是要 將C D資料與透鏡像差之”特徵(signature)"相關聯並不是一 件簡單的工作。因此,已經盡力進行透鏡像差之直接觀測 。舉例來說,由 Toh等人所著’’Identifying and Monitoring of Lens Aberrations in Projection Printing”,SPIE Vol. 772 — 書中,ρρ·202·209(1987)使說明一種測量約略0.2 λ之較大 型透鏡像差之效應的方法,其中λ係曝光波長。然而,現 今之近-繞射-限制光學設備中,大部分的像差都在0.05 λ附 近,或更小。以130nm特徵而言,當利用KrF曝光源時0.05 λ透鏡像差會轉變成12.4nm的誤差。因此,如果該特徵CD 的誤差範圍(換言之誤差容限值)假設為目標特徵寬度的 ±10%的話,12.4nm的誤差便幾乎是整個CD的誤差範圍。 在 Gortych等人所著’’Effects of Higher-Order Aberrations on the Process Window",SPIE Vol· 1463 —書中,ρρ·368_ 381 (1991)說明高階(higher-order)透鏡像差可能使微影過程 視窗惡化。不幸地,在裝配微影系統之後該高-透鏡像差非 常難以 /肖除。在 Brunner 所著 ’’ Impact of Lens Aberration on Optical Lithography,,,一 書中,INTERFACE 1996 Proceedings,ρρ·;μ27(1996)利用模擬解釋由數個第一階透 -9- 本纸張尺度適用中國國家檩準(CNS) Α4規格(210 X 297公釐) 1239434 A7 B7 五、發明説明(7 ) 鏡像差所產生之近-波長特徵的負面影響。特別的是,當利 用衰減式PSM時藉由檢查如何印刷接觸點特點便可以觀測到 馨形像差(coma aberrations)。同時已經知道藉由客製的離軸 照明可以平衡透鏡像差。已經努力試圖量測各種透鏡像差 以達成更佳的CD控制。 由 F arrar 等人戶斤著” Measurement of Lens Aberrations Using an In-Situ Interferometer Reticle ,’’ 一書中, Advanced Reticle Symposium,San Jose,CA. (June 1999)提 出可以使用原位置(in situ)干涉計標線(interferometer reticle)直接測量透鏡像差。根據Farrar的論點,可以推論高 達3 7個澤尼克(Zernike)之透鏡像差。雖然Farrar聲稱該方法 係準確並且可重複的,不過其包含了上百種或上千種登記 型式之測量方法(換言之量測與預期特徵位置有關之偏移)。 因此,Farrar的方法雖然準確並且可以重複,但是需要繁複 的測量,所以很清楚地該方法係非常消耗時間,因此可能 不適用於製造導向(manufacturing-driven)的環境中。此外, 可理解的是為了各種原因必須隨著時間記錄透鏡像差(例如 可以在系統中執行定期預防保養)。因此,定期監視透鏡效 能相當的重要,所以Fanrar的方法,其需要大量的測量及計 算,並不實用。因此,需要有一種可以直接從印刷產品晶 圓監視透鏡像差的方法。 為了達成此目標,Dirksen等人(參見,舉例來說,PCT專 利申請案W0 〇〇/3 1592)提出一種直接從印刷晶圓監視〇透鏡 像差之方法。根據Dirksen的方法,該透鏡監視包括標線上 -10- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 1239434 A7 B7 五、發明説明(8 簡單的圓形特徵。更特別的是,該圓形特徵係蝕刻至該標 線玻璃基板之無色特徵(chromeless)。姓刻深度通常為又/2 而直徑約略為(又/NA),其中N A係為投影透鏡之數字孔徑 。根據Dirksen的論點,該方法已被證實為有效的。此外, 該結構相當簡單並且夠小可以輕易地放置在整個曝光範圍 中〇 還有,還有一些關於使用Dirksen之透鏡像差監視的問題 。首先,該光罩上透鏡監視特徵之深度必須蝕刻至大約為 該波長之一半。對特殊用途之光罩來說,使用額外的(或特 殊的)光罩製程步驟以製造此類特徵並不會有問題。然而, 對生產標線型式來說,例如雙黃標線或attPSM,需要額外 光罩製程步驟以進行監視便是一種昂貴而且耗時的過程。 交替式PSM( altPSM)或非黃色PSM( CLM)也需要該額外光罩 製程步驟。此外,當對抗7Γ·相位時,因為Dirksen監視必須 在石英基板產生不同的蝕刻深度,因此需要特殊的蝕刻時 間並且必須分開進行。 使用Dirksen透鏡監視的第二個問題是難以防止因為光罩 形成期間石英蝕刻過程所引起的相位誤差。更特別的是, 參考圖式1 (a) -1 ( f)(其中S表示石英光罩基板),對惡化的 相位誤差來說,該石英蚀刻過程會在該光罩上產生斜邊形 狀,如圖1(a)所示。在此類實例中,該Dirksen監視失去顯 示任何可能之透鏡像差的敏感度。然而,如果在該光罩上 沒有相位誤差的話’如圖1 (d)所示,該Dirksen監視便可以 有效地偵測透鏡像差。圖1 (b)及1 (e)所示的分別係圖1 ( a) -11 - 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐)1239434 A7 B7 5. Description of the invention (3) Etchant) The target position (for example, including one or more crystal grains) on the substrate (silicon wafer). Generally speaking, a single wafer will contain adjacent target parts, which are irradiated through the projection system one at a time to the entire network. In the current device, patterning is performed using a mask on a mask platform to distinguish between different machine types. In one of the lithographic projection devices, each target position is irradiated by exposing a positive mask pattern to the target position. This type of device is generally called a wafer stepper. In the alternative device, a general step is a step-and-scan device. The irradiation of each target part is performed progressively in a predetermined reference direction (" scan " direction) under the projection beam. Scan and simultaneously scan the substrate platform in a direction parallel to or in the opposite direction; because, usually, the projection system has a magnification factor (usually < 1), so the speed V of scanning the substrate platform is to scan the mask platform M times the speed. More information on the lithographic devices described herein can be found in US 6,046,792 ', which is hereby incorporated by reference. In such a manufacturing process using a lithographic projection device, a pattern in a photomask (or other pattern member) is mapped onto a substrate at least partially covered with a photosensitive material (resist). Prior to this mapping step, the substrate is subjected to various procedures, such as priming, resist application, and soft baking (SOBake). After the exposure, the substrate is subjected to other procedures such as post-exposure bake (PEB), development, hard bake, and mapping feature measurement / inspection. This program is used as a basis for patterning of individual layers of a device ', such as an integrated circuit (1C). Then such a patterned layer will undergo various procedures such as etching, ion implantation (doping), metallization, oxidation, chemical-mechanical polishing, etc. All procedures are intended to complete a -6-1239434 A7 B7 5 2. Description of the invention (4) Other layers. If several layers are needed, the entire process, or its changes, must be repeated for each new layer. Finally, an array of devices is presented on the substrate (wafer). These devices are then separated from each other using techniques such as dicing or sawing, so individual devices can be mounted on a carrier, connected to pins, and so on. Further information on such procedures can be found in "Microchip Fabrication: A Practical Guide to Semiconductor Processing" by Peter van Zant, third edition, published by McGraw Hill Publishing Co. in 1997 ISBN 0-07-067250-4— Obtained from the book. For the sake of simplicity, the projection system will hereinafter be referred to as the n-lens π; however, this proper term should be generally interpreted as including various types of projection systems, including, for example, refractive optical systems, Reflective optical systems, and catadioptric systems. The illumination system also includes elements that operate according to any design pattern to guide, shape, or control the illumination projection beam, and such elements are also referred to below as '' lens". In addition, the lithographic apparatus may be of a type having two or more substrate platforms (and / or two or more photomask platforms). In this type of `` multi-stage '' device, the additional platform can be used simultaneously, with preparation steps on one or more platforms, and one or more other platforms used as exposure. For example, a two-stage lithography device is used in It is described in US 5,969,441 and WO 98/40791, which are hereby incorporated by reference. The current state of IC manufacturing requires a lithography program to provide the pattern feature line width close to one-half of the exposure wavelength. For a 150nm device, KrF excimer laser (DUV; 248nm) is usually selected as the exposure. The paper size is applicable to the Chinese National Standard (CNS) A4 specification (210 X 297 mm) 1239434 A7 B7 V. Source of invention description (5). Recent research and development can already use KrF excimer lasers in 130nm devices. This can be achieved using multiple resolution enhancement techniques (RET), such as attenuated phase shift masks (attPSM) and off-axis (off -axis) illumination (ΟΑΙ), combined with optical proximity correction (OPC) technology. A shorter exposure wavelength can be used instead of the above technology , Such as an ArF excimer laser with a wavelength of 193 nm, or using a lens with an ultra-high digital aperture (NA), such as NA = 0.8 or larger. However, these alternative technologies require a large capital investment in new devices And, if feasible, generally want to delay such expenditures. Therefore, integrated component manufacturers generally want to get the most out of existing DUV systems before switching to replacement equipment. Regardless of what is used in the manufacturing process Excimer lasers, manufacturing devices with critical dimensions of 150nm or less require near-diffraction-limited lenses used in the manufacturing process to have no aberrations. As is well known, aberrations can be Caused by various sources, such as defective lenses, or aging lasers, the frequency of their beams has shifted from the desired value. Therefore, it is desirable to check the lens performance before the device (in other words, verify the lens), and then during use ( For example, during the IC manufacturing process) monitor the lens performance. During the lens manufacturing process, the lens performance can be interfered with A complete test is performed interferometrically. Usually, the lens is first verified in the factory, and then re-verified when it is first installed in the field. A method commonly used to verify the lens is to print the wafer and then measure the minimum feature width, or Critical Dimension (CD). During the verification process, the paper size will apply to the Chinese National Standard (CNS) A4 (210 X 297 mm) 1239434 A7 B7. 5. Description of the invention (6) Measurement "vertical "And" horizontal "features (in other words, features extending in two orthogonal directions on the substrate plane, such as along the X and Y axes). In some instances, CDs with 45 degree features are also measured. To check the effectiveness of the lens, a sufficient number of CD measurements must be made throughout the exposure. The results of the CD measurements are then analyzed to determine if the lens's performance is acceptable. Although the CD measurement method provides a method for evaluating lens performance, it is not a simple task to correlate CD data with the "signature" of lens aberrations. Therefore, efforts have been made to directly observe lens aberrations For example, "Identifying and Monitoring of Lens Aberrations in Projection Printing" by Toh et al., SPIE Vol. 772 — In the book, ρ · 202 · 209 (1987) makes it possible to explain a larger measurement of approximately 0.2 λ Method of the effect of lens aberrations, where λ is the exposure wavelength. However, in today's near-diffraction-limited optical devices, most of the aberrations are around 0.05 λ or less. In terms of 130nm characteristics, when using a KrF exposure source, the 0.05 λ lens aberration will be transformed into an error of 12.4nm. Therefore, if the error range of the feature CD (in other words, the error tolerance value) is assumed to be ± 10% of the target feature width, the error of 12.4nm is almost the error range of the entire CD. In "Effects of Higher-Order Aberrations on the Process Window" by Gortych et al., SPIE Vol. 1463-book, ρ · 368_ 381 (1991) shows that higher-order lens aberrations may cause lithographic processes The window deteriorated. Unfortunately, this high-lens aberration is very difficult to remove after the lithography system is assembled. In the book `` Impact of Lens Aberration on Optical Lithography, '' by Brunner, INTERFACE 1996 Proceedings, ρρ; μ27 (1996) uses simulations to explain from several first-order transmissions. 9- This paper scale applies to China National Standards (CNS) A4 specification (210 X 297 mm) 1239434 A7 B7 V. Description of the invention (7) Negative effect of near-wavelength characteristics due to mirror image difference. In particular, when using the attenuated PSM, coma aberrations can be observed by examining how the contact point characteristics are printed. It is also known that lens aberration can be balanced by custom off-axis illumination. Efforts have been made to measure various lens aberrations to achieve better CD control. In the book "Measurement of Lens Aberrations Using an In-Situ Interferometer Reticle" by Farrard et al., Advanced Reticle Symposium, San Jose, CA. (June 1999) proposed that in-situ interference can be used. Interferometer reticle directly measures lens aberrations. According to Farrar's argument, lens aberrations of up to 37 Zernike can be inferred. Although Farr claims that the method is accurate and repeatable, it includes Hundreds or thousands of registration types of measurement methods (in other words, measuring the offset related to the expected feature position). Therefore, although Farrar's method is accurate and repeatable, it requires complicated measurements, so it is clear that this method is very It is time consuming and therefore may not be suitable for a manufacturing-driven environment. In addition, it is understandable that lens aberrations must be recorded over time for various reasons (for example, regular preventive maintenance can be performed in the system). Therefore, It is important to regularly monitor lens performance, so Fanrar's method requires Measurement and calculation of quantities are not practical. Therefore, there is a need for a method that can monitor lens aberrations directly from printed product wafers. To achieve this goal, Dirksen et al. (See, for example, PCT patent application WO 0). 〇 / 3 1592) proposed a method for monitoring lens aberrations directly from printed wafers. According to Dirksen's method, the lens monitoring includes the marking line -10- This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 (Mm) 1239434 A7 B7 V. Description of the invention (8 Simple circular feature. More specifically, the circular feature is etched to the chromeless of the graticule glass substrate. The depth of the engraving is usually / 2. The diameter is approximately (also / NA), where NA is the digital aperture of the projection lens. According to Dirksen's argument, this method has been proven to be effective. In addition, the structure is quite simple and small enough to be easily placed throughout the exposure In the range, there are also some questions about the lens aberration monitoring using Dirksen. First, the depth of the lens monitoring feature on the reticle must be etched to about the wave One and a half long. For special-purpose masks, it is not a problem to use additional (or special) mask process steps to make such features. However, for production line types, such as double yellow labels Line or attPSM, requiring additional photomask process steps for monitoring is an expensive and time-consuming process. Alternate PSM (altPSM) or non-yellow PSM (CLM) also requires this additional photomask process step. In addition, when confronting the 7Γ · phase, because Dirksen monitoring must produce different etching depths on the quartz substrate, special etching time is required and must be performed separately. A second problem with Dirksen lens monitoring is that it is difficult to prevent phase errors due to the quartz etching process during the mask formation. More specifically, referring to Figure 1 (a) -1 (f) (where S represents a quartz mask substrate), for a deteriorated phase error, the quartz etching process will produce a beveled shape on the mask, As shown in Figure 1 (a). In such examples, the Dirksen monitor loses its sensitivity to show any possible lens aberrations. However, if there is no phase error on the mask, as shown in Fig. 1 (d), the Dirksen monitoring can effectively detect lens aberrations. Figures 1 (b) and 1 (e) are shown in Figure 1 (a) -11-This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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足傾斜’’ Dirksen監視結構及圖1(d)之”理想的”以^^⑶監 視結構所產生之印刷抗蝕劑圖案的橫切面。 應該注意的是®1(b)及1(e)中用以製造抗蝕劑形狀的印 刷狀況如下·具有〇·8局邵黏著於+ 〇1Vm失焦(de_f〇cus)之 0.68NA,在多晶矽晶圓上方有機BARC(AR2)上使用厚度〇4 的ShipleyUV6抗蝕劑。該模擬會在又&丫(27及28澤尼 克)產生+ 0.025又的彗形。 當更詳細檢查Dirksen監視結構所形成之環形抗蝕圖案時 ,如圖1 (c)及1 (f)所示之範例,可以清楚的看到該印刷抗 蝕圖案的内環具有較稀薄的抗蝕劑形狀與外環結構所形成 之陡峭形狀形成對比。此差異之原因係為外環抗蝕劑圖案 係由在光罩之相位改變所形成,而内環抗蝕劑圖案的形成 則沒有這類的相位改變。特別的是,該内環抗蝕劑圖案係 經由穿過Dirksen監視圖案中心之曝光波長衰減所形成。換 言之,該兩種抗蝕劑形狀(換言之内環及外環)係由兩種不同 的對數斜率(log-slope)所形成。抗蝕劑形狀的不同可能導致 錯誤的測量,其可能造成對討論中之透鏡像差的誤判。 應遠注意的是可以藉由Dirksen透鏡像差監視器觀測少量 之彗形,如圖1 (e )及(f)所示。特別的是,該環狀寬度在左 邊與右邊並不相同。尚得注意的是很難在”傾斜”之Dirksen 監視器中觀測此彗形,如圖1(b)及1(c)所示。 因此,基於上述之問題,仍然需要一種透鏡觀測器用以偵 測透鏡像差,但是卻不會因為光罩製程中輕微的缺陷而輕 易地遭到損壞。也希望該透鏡監視器結構夠小可以放置在 12- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 1239434 A7The foot-tilt '' Dirksen monitor structure and the "ideal" cross-section of the printed resist pattern produced by the structure in Fig. 1 (d) are monitored with ^^ ⑶. It should be noted that the printing conditions used to make resist shapes in ®1 (b) and 1 (e) are as follows: · With 0.8 cycles of adhesion to + 〇1Vm defocus (de_f〇cus) of 0.68NA, A Shipley UV6 resist with a thickness of 4 is used on an organic BARC (AR2) over a polycrystalline silicon wafer. This simulation will produce + 0.025 coma at y & y (27 and 28 zenik). When the ring-shaped resist pattern formed by the Dirksen monitoring structure is examined in more detail, as shown in the examples shown in Figures 1 (c) and 1 (f), it can be clearly seen that the inner ring of the printed resist pattern has a thinner resistance. The shape of the etch contrasts with the steep shape formed by the outer ring structure. The reason for this difference is that the outer ring resist pattern is formed by a phase change in the mask, while the inner ring resist pattern is formed without such a phase change. In particular, the inner ring resist pattern is formed by attenuation of the exposure wavelength through the center of the Dirksen monitor pattern. In other words, the two resist shapes (inner and outer rings) are formed by two different log-slopes. Differences in the shape of the resist may lead to erroneous measurements, which may cause misjudgment of the lens aberrations in question. It should be noted that a small amount of coma can be observed by the Dirksen lens aberration monitor, as shown in Figures 1 (e) and (f). In particular, the width of the ring is not the same on the left and right. It should also be noted that it is difficult to observe this coma in a "tilted" Dirksen monitor, as shown in Figures 1 (b) and 1 (c). Therefore, based on the above problems, a lens viewer is still needed to detect lens aberrations, but it will not be easily damaged due to slight defects in the mask manufacturing process. It is also hoped that the lens monitor structure is small enough to be placed in 12- This paper size applies to China National Standard (CNS) A4 specifications (210X 297 mm) 1239434 A7
五、發明説明(W 生產晶^間或旁邊以進行現場監视 额外光罩製程步驟便可以製造該透鏡監視$。也希4^ 為努力解決上述之需求,本發明的目的:―便是提供 具觀測透鏡像差能力之透鏡龄# ’、 ^ 延貌皿視斋。本發明之另一目 該透鏡監視器的像差分析社摄約^ & 1 ^ 刀斫、、、口構夠小使該監視器可以作現与 監視。此外,本發明的目的之_ 係不而要額外的製程步屬 便可以製造孩監視器,例如在朵¥ J如在先罩形成期間,並且該透頷V. Description of the Invention (The lens monitor can be manufactured by manufacturing the additional mask steps on or next to the wafer for on-site monitoring. Also hope that in order to solve the above-mentioned needs, the purpose of the present invention is to provide Lens age with observation lens aberration capability # ', ^ Yanmao Dianshizhai. Another lens of the present invention, the aberration analysis agency of the lens monitor, about ^ & 1 The monitor can be used to monitor and monitor. In addition, the purpose of the present invention is to make a child monitor without additional process steps, for example, during the formation of the front cover, and the transparency
監視器的功能不會因為光罩製昶由 疋早I%中輕微的缺陷而明顯地ϋ 到損壞。 訂The function of the monitor will not be significantly damaged by a slight defect in the early I% due to the mask mechanism. Order
更特別的是,本發明係關於用以—種用以偵測透鏡像差之 透鏡像差監視器。該監視器包括多個無法分解之特徵(舉例 來說’配置在光罩上)。該多個無法分解特徵係用以在該基 板上投影預設的測試圖案’接著利用該測試圖案偵測透鏡 像差。監視器大小必須可以放入該微影裝置以及裝置圖的 目標區中,相當於在該基板上形成一種裝置(例如積體電路) ,舉例來#,该監視器必須夠小以安裝包含I c圖案之光罩 本發明也係關於一種觀測與使用於該公開文章中之光學微 影系統中之光學系統(照射系統以及/或是投影透鏡)相關聯 的像差的方法。在内文中,該方法包括的步驟有: -1¾:供該所要的圖案以包括一個具有多個無法分解特徵監 視器,其中該多個無法分解特徵係用以在投影該基板時 形成預設的圖案; -利用該投影系統將該監視投影在該基板上;及 -13- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 1239434More specifically, the present invention relates to a lens aberration monitor for detecting lens aberration. The monitor includes a number of features that cannot be disassembled (for example, 'located on a reticle). The plurality of non-decomposable features are used to project a preset test pattern on the substrate and then use the test pattern to detect lens aberrations. The size of the monitor must fit into the target area of the lithography device and the device map, which is equivalent to forming a device (such as an integrated circuit) on the substrate. For example, the monitor must be small enough to be installed to contain I c Patterned mask The present invention also relates to a method for observing aberrations associated with an optical system (illumination system and / or projection lens) used in the optical lithography system used in the publication. In the text, the method includes the steps of: -1¾: for the desired pattern to include a monitor having a plurality of non-decomposable features, wherein the plurality of non-decomposable features are used to form a preset when projecting the substrate. Pattern;-use the projection system to project the surveillance on the substrate; and -13- this paper size applies Chinese National Standard (CNS) A4 specification (210X 297 mm) 1239434
-分析該預設試驗圖案之位置及該監視器中多個無法分解 之特欲的位置以判斷是否產生像差。 除了該監視器,該所希望之圖案尚包括一元件圖案,相當 於在該基板上形成一積體元件層。 如下面所解釋,如果預設測試圖案之位置與預期的位置不 同時,其係從該多個無法分解特徵中判斷,與預期位置之 偏移便表示像差的存在。 如下面更進步的詳細說明,本發明提供明顯超過先前技 藝之優點。更重要的是,本發明提供—種具有偵測非常細 微透鏡像差能力之透鏡監視器。此外,因為該透鏡監視器 結構之全邵尺寸非常地小,所以該監視器結構可以放置在 非常多的位置以監視整個曝光範圍。 如果該監視器係放置在光罩上的話,那麼便不會受到用以 形成該監視器之光罩形成製程缺陷的影#。在此類實例中 ,本發明《透鏡監视器適合進行現場監視,因為該透鏡監 視器可以利用與形成該生產光罩相同的光罩形成製程來ς 成,因此不需要任何額外的光罩形成製程步驟。另一項優 點係該透鏡監視器的有效性比較不會受到該光罩製程本身 的,,傾斜”相位邊緣及,,角邊圓滑(corner r〇unding) ”效應 響。 #、 熟習此技蟄义人士可以從下面的圖式及隨附的本發明具體 貫例之細部說明中更解本發明之其它優點,其中·· 圖所示的係,,傾斜的” Dirksen透鏡像差'監視器結構之 上方及剖面圖。 -14--Analyze the position of the preset test pattern and a number of unintended positions in the monitor to determine whether aberrations have occurred. In addition to the monitor, the desired pattern includes an element pattern, which is equivalent to forming an integrated element layer on the substrate. As explained below, if the position of the preset test pattern is different from the expected position, it is judged from the plurality of unresolvable features, and the deviation from the expected position indicates the existence of aberrations. As described in more detail below, the present invention provides significant advantages over previous techniques. More importantly, the present invention provides a lens monitor with the ability to detect very fine lens aberrations. In addition, because the overall size of the lens monitor structure is very small, the monitor structure can be placed in a large number of positions to monitor the entire exposure range. If the monitor is placed on a mask, it will not be affected by the defects in the mask formation process used to form the monitor. In such examples, the lens monitor of the present invention is suitable for on-site monitoring because the lens monitor can be formed using the same mask forming process as the production mask, so no additional mask formation is required. Process steps. Another advantage is that the effectiveness of the lens monitor is relatively unaffected by the mask process itself, the "tilted" phase edges and, "corner rounding" effects. # 、 Those who are familiar with this technique can further understand the other advantages of the present invention from the following drawings and the detailed description of the specific implementation examples of the present invention. Among them, the system shown in the figure, the inclined "Dirksen transparent Above and sectional view of the mirror image difference monitor structure. -14-
1239434 A7 B7 五、發明説明(12 ) 圖Ub)所示的係由圖1(a)之”傾斜的” Dirksen透鏡像差監 視為結構所產生之印刷抗蝕圖案之剖面圖。 圖Uc)所示的係圖1(b)中抗蝕圖案之俯視圖。 圖1 (d)所示之係”理想的” Dirksen透鏡像差監視器結構之 上方及剖面圖。 圖He)所示的係由圖1(d)之”理想的” Dirksen透鏡像差監 視器結構所產生之印刷抗蝕圖案之剖面圖。 圖UO顯示圖1(e)所示之抗蝕圖案之俯視圖。 圖2(a)所示的係修正Dirksen監視器結構以形成似環狀 (ring-like)結構之剖面圖。 圖2(b)所示的係圖2(a)中似環狀結構之一維剖面空間影 像。 / 圖2(c)所示的係圖2(a)中似環狀監視器結構所產生之印 刷抗蝕圖案之剖面圖。 圖3 (a)所示的係根據本發明之透鏡像差監視器結構之範 例0 圖3 (b)-3(g)所示的係圖3(a)中透鏡像差監視器結構之變 化以及其印刷效能範例。 圖4(a)所示的係由圖1中Dirksen監視器結構所產生之物件 相位光譜。 圖4(b)所示的係由圖2中,,似環狀,’監視器結構所產生之物 件相位光譜。 圖4(c)所示的係由圖3(a)中透鏡像差監视器結構所產生 之物件相位光譜。 -15-1239434 A7 B7 V. Description of the invention (12) Figure Ub) is a cross-sectional view of the printed resist pattern produced by the "diagonal" Dirksen lens aberration of Figure 1 (a) as a structure. Figure Uc) is a top view of the resist pattern in Figure 1 (b). The top and cross-sectional views of the "ideal" Dirksen lens aberration monitor structure shown in Figure 1 (d). Figure He) is a cross-sectional view of a printed resist pattern produced by the "ideal" Dirksen lens aberration monitor structure of Figure 1 (d). FIG. UO shows a top view of the resist pattern shown in FIG. 1 (e). Figure 2 (a) is a cross-sectional view of a modified Dirksen monitor structure to form a ring-like structure. Fig. 2 (b) is a one-dimensional cross-sectional spatial image of the ring-like structure in Fig. 2 (a). / Fig. 2 (c) is a cross-sectional view of a printed resist pattern produced by a ring-like monitor structure in Fig. 2 (a). An example of the structure of a lens aberration monitor according to the present invention shown in FIG. 3 (a) is shown in FIG. 3 (b) -3 (g). And examples of their printing performance. Figure 4 (a) shows the phase spectrum of the object generated by the structure of the Dirksen monitor in Figure 1. The phase spectrum shown in Fig. 4 (b) is the phase spectrum of the object produced by the "ring-like" monitor structure in Fig. 2. The phase spectrum of the object shown in Figure 4 (c) is generated by the lens aberration monitor structure in Figure 3 (a). -15-
1239434 A7 —______ B7_ 五、發明説明(13 )1239434 A7 —______ B7_ V. Description of the invention (13)
圖4(d)所示的係由圖1中Dirksen監視器結構所產生之1-D 剖面空間影像。 圖4(e)所示的係由圖2中,,似環狀”監視器結構所產生之^ D剖面空間影像。 圖4(f)所示的係由圖3(a)中透鏡像差監視器結構所產生之 1 -D剖面空間影像。 圖5 (a) - 5 (c)所示的係圖3 (a)中透鏡像差監視器結構之實 際印刷效能。 圖6(a)所示的係圖3 (a)中透鏡像差監視器結構之上方及 剖面圖,其中該光罩形成過程會導致具有傾斜邊緣之無法 分解特徵。 圖6(b)所示的係圖6(a)中透鏡像差監視器結構所產生之 物件相位光譜。 圖6(c)所示的係藉由投影透鏡投影之圖6(a)中透鏡像差 監視器結構之二維空間影像。 圖6 ( d)所示的係與印刷在晶圓上之透鏡像差監視器結構 重疊之圖6(a)中原始抗蝕圖案之俯視圖。 圖6(e)所示的係符合圖6(a)之監視器結構之透鏡像差監 視器結構之剖面圖。 圖7(a)-7(d)所示的係與6〇/〇 attpsM或雙黃光罩一起使用 之本發明的透鏡像差監視器的能力。 圖8 (a)-8(h)所示的係用以偵測透鏡像差之本發明的透鏡 像差監視器的能力。 圖9描述的係適用本發明之微影投影裝置。 -16-Figure 4 (d) is a 1-D cross-sectional spatial image generated by the Dirksen monitor structure in Figure 1. The system shown in Fig. 4 (e) is a ^ D cross-sectional spatial image generated by the "ring-like" monitor structure in Fig. 2. The system shown in Fig. 4 (f) is based on the lens aberration in Fig. 3 (a). The 1-D cross-section spatial image produced by the monitor structure. Figures 5 (a)-5 (c) are the actual printing performance of the lens aberration monitor structure shown in Figure 3 (a). Figure 6 (a) The top and cross-sectional views of the lens aberration monitor structure shown in Fig. 3 (a), in which the photomask formation process results in an indecomposable feature with a slanted edge. Fig. 6 (a) The phase spectrum of the object produced by the lens aberration monitor structure shown in Figure 2). Figure 6 (c) is a two-dimensional spatial image of the lens aberration monitor structure of Figure 6 (a) projected by a projection lens. Figure 6 (d) The top view of the original resist pattern in Fig. 6 (a), which overlaps the structure of the lens aberration monitor printed on the wafer. The system shown in Fig. 6 (e) corresponds to Fig. 6 (a). Sectional view of the lens aberration monitor structure of the monitor structure. Figure 7 (a) -7 (d) shows the lens aberration monitor of the present invention used with 60 / attsM or double yellow mask. Device capabilities. Figure 8 (a The capability of the lens aberration monitor of the present invention for detecting lens aberrations shown in -8 (h) is shown in FIG. 9. The lithographic projection apparatus to which the present invention is applied is described in FIG. -16-
本紙張尺度適用中國國豕標準(CMS) A4規格(210 X 297公董) 1239434 A7 B7 五、發明説明( 14 ) 在該些圖式中,相同特徵係以相同的參考符號表示。 主要元件符號說明 10 透鏡像差監視器結構 12 次解析特徵(或八個正方形特徵) 12a-12d 特徵 14 内環 15 外環 16 (印刷OHR結構左側)内部 17 (印刷OHR結構右側)内部 AM 調整構件 C 目標部份 CO 聚光器 Ex 照射系統 IF 定位構件 IL 照射系統(或照明器) IN 整合器 LA 照射源 MA 光罩 MT 第一物件平台(光罩平台) PB 投影光束 PL 投影系統 W 基板 WT 第二物件平台(基板平台) 下列本發明之透鏡像差監視器的詳細說明係關於透鏡像差 -17- 本紙張尺度適用中國國家標準(CNS) A4規格(210 x 297公釐) 1239434 A7 B7 五、發明説明(15 ) 本身,及形成該監視器之方法。應該注意的是,為使更容 易了解本發明,下列將會詳述如何利用該監视器在光罩上 形成環狀結構。然而,也應該注意的是本發明並非僅限於 此類環狀結構;明確地說,也可以有其它形狀。此外,該 結構不需要一定在光罩上形成;它們可以,舉例來說,使 用其它圖案構件產生。 從上述關於Dirksen監視恭之觀測中,本發明之發明人最 初的想法認為Dirksen監視器結構的内環抗蝕形狀可以藉由 修改監視器使其呈現似環狀結構而予以改善。換言之, Dirksen監視器結構内環之減少的/稀薄的抗蚀形狀可以藉由 在違結構的中心點產生相位改變而加以改正。然而,與最 初的想法相反,本發明之發明人判斷出在Dirksei^#構中心 點產生相位改變並不會造成呈現似環狀結構之抗蝕形狀。 此外,所產生的抗蝕形狀實質上並無法監視透鏡像差。 圖2(a)-2(c)所示的係修改〇11:1^611監視器結構以形成似環 狀結構。特別的是,圖2(a)所示的係修改Dirkser^#構以形 成似環狀結構之上方及剖面圖。圖2(b)係圖2(a)(其中工表 示強度)之似環狀結構的一維剖面空間影像。圖2(c)係由圖 2 (a)中似環狀結構所產生之印刷抗蝕圖案之剖面圖。從圖 2(a)-2(c)中可以清楚得知,該似環狀結構(圖並不會 產生環狀抗蝕形狀。這是因為該監視器結構之空間影像^ 比不夠強烈以形成”似環狀,,抗蝕結構。結果,圖2(昀之結 構實質上並無法用以監視器透鏡像差。值得注意的是只要 該監視器結構的直徑在又/NA範圍中的話,前面的方法係 -18-This paper size applies to the Chinese National Standard (CMS) A4 specification (210 X 297 public directors) 1239434 A7 B7 V. Description of the invention (14) In these drawings, the same features are indicated by the same reference symbols. Key component symbol description 10 Lens aberration monitor structure 12 times analytical features (or eight square features) 12a-12d features 14 Inner ring 15 Outer ring 16 (on the left side of printed OHR structure) Inside 17 (on the right side of printed OHR structure) Internal AM adjustment Component C Target part CO Concentrator Ex Illumination system IF Positioning component IL Illumination system (or illuminator) IN Integrator LA Illumination source MA Mask MT First object platform (mask platform) PB Projection beam PL Projection system W Substrate WT Second Object Platform (Substrate Platform) The following detailed description of the lens aberration monitor of the present invention is related to the lens aberration -17- This paper size applies to China National Standard (CNS) A4 (210 x 297 mm) 1239434 A7 B7 V. Description of Invention (15) itself, and method of forming the monitor. It should be noted that in order to make the present invention easier to understand, the following will detail how to use the monitor to form a ring structure on a photomask. However, it should also be noted that the present invention is not limited to such a ring structure; specifically, other shapes are also possible. Furthermore, the structures need not necessarily be formed on a reticle; they can, for example, be produced using other pattern members. From the above observations on the Dirksen monitoring, the original idea of the inventors of the present invention is that the shape of the inner ring corrosion resistance of the Dirksen monitor structure can be improved by modifying the monitor so that it presents a ring-like structure. In other words, the reduced / thinner resist shape of the inner ring of the Dirksen monitor structure can be corrected by generating a phase change at the center point of the offending structure. However, contrary to the original idea, the inventors of the present invention have determined that a phase change at the center point of the Dirksei ^ # structure does not cause a resist shape that exhibits a ring-like structure. In addition, the resulting resist shape does not substantially monitor lens aberrations. The system shown in Figs. 2 (a) -2 (c) modifies the monitor structure of 11: 1 ^ 611 to form a ring-like structure. In particular, the system shown in Fig. 2 (a) is modified by the Dirkser ^ # structure to form a ring-like structure above and in a cross-sectional view. Fig. 2 (b) is a one-dimensional cross-sectional space image of a ring-like structure in Fig. 2 (a) (where the intensity is shown). Fig. 2 (c) is a cross-sectional view of a printed resist pattern produced by the ring-like structure in Fig. 2 (a). It can be clearly seen from Figs. 2 (a) -2 (c) that the ring-like structure (the figure does not produce a ring-shaped resist shape. This is because the spatial image ratio of the monitor structure is not strong enough to form "Loop-like, corrosion-resistant structure. As a result, Figure 2 (the structure of 昀 can not be used to monitor lens aberrations in essence. It is worth noting that as long as the diameter of the monitor structure is in the / NA range, the front Methodology
1239434 A7 —_____B7 I、發明説明(16 ) — "~' 相當準確的。對一較大直徑而言,圖2 (a)之似環狀設計可 能印刷出一似環狀之抗蝕圖案。然而,當直徑超過;i /NA 時’透鏡像差監視之效應便會減少。 綜觀上述,本發明主要目的之一係提供一有效直徑在入 /Ν Α範圍中結構之透鏡像差監視器,其產生一空間影像具 有對數斜率斜度足以充分感應表示透鏡像差。 圖3 ( a)所示的係根據本發明之透鏡像差監視器結構丨〇之 範例。如圖中所示,該透鏡像差結構1 〇,其係參考八網版 環(Octad Halftone Ring,OHR),係一次解晰之網版結構包 括多個次解晰特徵1 2。次解晰網版結構形成之詳細討論如, 舉例來說,歐洲專利申請文編號EP 〇 980 542中所提出的。 在圖3 (a)所示之具體實例中,該次解晰網版結構丨〇之所 有形狀皆為圓形,而每一特徵1 2則為正方形。要注意的是 本發明之像差監視器結構1 〇並不僅限於此類形狀。無疑地 ,該次解晰網版結構1 0之全部形狀可以不是圓形,而每一 特徵1 2的形狀則可以不是正方形。要注意的是該正方形次 解晰特徵1 2在實際設計中會因為光罩製程的特性而很可能 變成角邊圓滑狀。 參考圖3 (a) ’個別之特徵1 2的尺寸及特徵1 2之間的間隔 如下所述。在一具體實例中,該正方形特徵之每邊尺寸s L 係約略為0.3(λ/ΝΑ)或更小。要注意的是該光罩製造解析會 限制次解晰特徵1 2之最小尺寸。以目前光罩製程而言,在 4X光罩上該解析限制係約略為2〇〇ηηι。在1 X晶圓刻度中, 相當於50nm。舉例來說,當利用0.68ΝΑ步進器以及KrF曝 -19- 本紙張尺度適用中國國家標準(CNS) A4規格(210X 297公釐) 1239434 A7 ___ _ B7 五、發明説明(17 ) 光源時,每一正方形特徵12之每邊尺寸可能約略在1〇〇11. 12Onm。為了維持網版的充分效果,最好的是在每方形特徵 12間之空間ES小於〇·15(λ/ΝΑ)。二選一,每一正方形特徵 1 2之間的間隔E S應該小於〇· 15(几/ΝΑ)。另外,每一特徵i 2 之間的間隔應該小於該正方形特徵1 2側邊尺寸的一半。要 注意的是,如圖3 ( a)所示,上述之空間條件所指的是鄰近 特徵1 2之間的間隔。另外要注意的是,如圖3 (a)所示,在 X及Y方向的交錯補償(staggered offset)(分別是XST及YST) 最好是相同。換言之,特徵12重疊X方向或γ方向上鄰近特 徵1 2的邵分最好是相同。在目前的具體實例中,該較佳的 交錯補償最好是在約略為該次解晰元素尺寸的丨/4至3 /4的 範圍中。最後,再參考圖3(a),尚要注意的是在兩個相對 特徵之内側邊之間最遠的距離EES,沿著X方向(換言之特徵 12a,12b)或Y方向(換言之特徵12c,12d),最好約略等於( λ /NA)。所有尺寸係以1 X晶圓刻度來表示。 在圖3(a)所示之透鏡像差監視器具體實例中,本發明之 次解晰網版結構1 0在似環狀格式中利用八個正方形特徵1 2 。然而,如已說明的,本發明不希望受限於此。無疑地, 可以產生並且利用並非呈現似環狀形狀之次解晰網版結構 。因為可以利用正方形以外其它形狀的特徵,所以可以利 用數量為八個以外的多個次解晰特徵以形成該次解晰網版 結構。 更特別的是’雖然似條狀(1 in e - like)結構(例如一對平行 線)可以顯示某些型式之透鏡像差(例如彗形),但是為了捕 -20- 本紙張尺度適财S Η家鮮(CNS) A4規格(21GX297公董) ~ 1 1239434 A7 ;--- - B7 五、發明説明(18 ) 捉其它型式 <透鏡像差及對應的方向,因此仍希望形成一,, 似%狀結構。另外,因為每一特徵i 2係為次解晰,所以該 特殊开^/狀並不重要。该特倣丨2之尺寸及網版的間隔係更為 重要。圖3(b),3(c)及3(d)係可以用於形成監視器結構之 /入解晰特欲12之各種結構之範例。圖3(e),3(f)及3(g)所 不的分別係圖3(b),3(c)及3(d)中所示之監視器結構之之 T際印刷效能。所有曝光都係在相同的情況下,即在環狀 …、明0.68NA下執行(〇·6個内西格瑪及〇·8個外西格瑪,西格 瑪(〇0即所謂的黏著係數)。此外,在每一實例中,都故意 產生〇·〇5 λ的X及γ之彗形量。對全部三個實例中來說,該 添透叙像差可清楚地從顯示於圖3 (e) , 3 ([)及3 ( $)之印 刷圖案中觀測到。 圖4卜)-4(〇所示的係1^1:]^611監視器結構(圖1),似環狀 監視器結構(圖2 )及本發明之0HR監視器結構(圖3 (a))之物 件光譜及空間影像之比較。在該些圖式中,p表示相位而工 ^示強度。更特別的是,首先參考圖4(a),所示的Dirksen 監視器之相位物件光譜在”N A(數字孔徑)限制範圍内並不 對稱。轉至圖4(b),所示的係該”似環狀”監視器具有對稱 之相位光譜但全部之相位範圍都被壓縮。然而,如上所解 釋及如圖4(e)所示,該”似環狀”監視器結構所呈現的空間 景> 像對比不夠,因此無法印刷出似環狀抗蝕圖案。 轉至圖4(c) ’所示的係該0HR監視器1〇在土να限制範圍 内呈現對稱的相位光譜,而全部相位範圍從〇至36〇度。當 在《0.3至0.35強度大小的印刷臨界處比較兩者時,該〇hr監 -21 - I紙張尺度適财_家鱗(⑽)A4規格(21GX297公爱) -------— 12394341239434 A7 —_____ B7 I. Description of the Invention (16) — " ~ 'is quite accurate. For a larger diameter, the ring-like design of Fig. 2 (a) may print a ring-like resist pattern. However, when the diameter exceeds i / NA, the effect of the lens aberration monitoring is reduced. In view of the foregoing, one of the main objects of the present invention is to provide a lens aberration monitor having an effective diameter in the range of N / A, which generates a spatial image with a logarithmic slope sufficient to sufficiently sense and represent the lens aberration. Fig. 3 (a) shows an example of a lens aberration monitor structure according to the present invention. As shown in the figure, the lens aberration structure 10 refers to the Octad Halftone Ring (OHR), and the screen structure of one resolution includes multiple resolution features 12. A detailed discussion of the formation of the secondary screen structure is, for example, proposed in European Patent Application No. EP 0 980 542. In the specific example shown in Fig. 3 (a), all the shapes of the stencil structure of this time are circular, and each feature 12 is square. It is to be noted that the aberration monitor structure 10 of the present invention is not limited to such a shape. Undoubtedly, the entire shape of the screen structure 10 may not be circular, and the shape of each feature 12 may not be square. It should be noted that the square secondary resolution feature 1 2 is likely to become rounded corners due to the characteristics of the mask process in actual design. Referring to FIG. 3 (a), the dimensions of the individual features 12 and the intervals between the features 12 are as follows. In a specific example, the size s L of each side of the square feature is approximately 0.3 (λ / NA) or less. It should be noted that this mask manufacturing analysis will limit the minimum size of the sub-resolution features 12. In terms of the current photomask manufacturing process, the resolution limit on a 4X photomask is about 200 nm. In a 1 X wafer scale, this is equivalent to 50 nm. For example, when using a 0.68 ΝΑ stepper and KrF exposure -19- this paper size applies Chinese National Standard (CNS) A4 specifications (210X 297 mm) 1239434 A7 ___ _ B7 V. Description of the invention (17) The size of each side of each square feature 12 may be approximately 100.12 Onm. In order to maintain the full effect of the screen, it is best that the space ES between 12 square features is less than 0.15 (λ / NA). Alternatively, the interval E S between each square feature 12 should be less than 0.15 (several / NA). In addition, the interval between each feature i 2 should be less than half the size of the side of the square feature 12. It should be noted that, as shown in Fig. 3 (a), the above-mentioned spatial conditions refer to the interval between adjacent features 12. Also note that, as shown in Figure 3 (a), the staggered offsets (XST and YST, respectively) in the X and Y directions are preferably the same. In other words, it is preferred that the features 12 that overlap the adjacent feature 12 in the X direction or the γ direction are the same. In the present specific example, the preferred interleaving compensation is preferably in the range of ¼ / 4 to 3/4 which is approximately the size of the resolution element. Finally, referring to Figure 3 (a) again, it should be noted that the farthest distance EES between the inner sides of two opposite features is along the X direction (in other words, features 12a, 12b) or the Y direction (in other words, feature 12c). , 12d), preferably approximately equal to (λ / NA). All dimensions are expressed on a 1 X wafer scale. In the specific example of the lens aberration monitor shown in Fig. 3 (a), the screen structure 10 of the present invention makes use of eight square features 12 in a ring-like format. However, as already explained, the present invention is not intended to be limited thereto. Undoubtedly, it is possible to generate and use sub-resolution screen structures that do not exhibit a ring-like shape. Because features of shapes other than squares can be used, multiple sub-resolution features other than eight can be used to form the sub-resolution screen structure. More special is' Although 1 in e-like structure (such as a pair of parallel lines) can display some types of lens aberrations (such as coma), S Η 家 鲜 (CNS) A4 specification (21GX297 public director) ~ 1 1239434 A7; ----B7 V. Description of the invention (18) Catch other types < lens aberrations and corresponding directions, so it is still desired to form one, , Like a% -like structure. In addition, because each feature i 2 is a sub-resolution, the special opening is not important. The size of the special imitation 2 and the spacing of the screens are more important. Figures 3 (b), 3 (c), and 3 (d) are examples of various structures that can be used to form the monitor structure. The differences between Figs. 3 (e), 3 (f), and 3 (g) are the T-printing performances of the monitor structures shown in Figs. 3 (b), 3 (c), and 3 (d), respectively. All exposures are performed under the same conditions, that is, in a ring ..., Ming 0.68NA (0.6 inner sigma and 0.8 outer sigma, sigma (0 is the so-called adhesion coefficient). In addition, in In each example, the coma amounts of X and γ of λ 0.05 were produced intentionally. For all three examples, the added aberration can be clearly seen from Fig. 3 (e), 3 ([) And 3 ($) were observed in the printed pattern. Figure 4b) -4 (〇 shown in the system 1 ^ 1:] ^ 611 monitor structure (Figure 1), like a ring monitor structure (Figure 2) Comparison of object spectrum and space image with the 0HR monitor structure of the present invention (Fig. 3 (a)). In these drawings, p represents the phase and the intensity is shown. More specifically, first refer to the figure 4 (a), the phase object spectrum of the Dirksen monitor shown is not symmetrical within the "NA (Digital Aperture) limit. Turning to Fig. 4 (b), the shown" ring-like "monitor has A symmetrical phase spectrum but the entire phase range is compressed. However, as explained above and shown in Figure 4 (e), the spatial landscape presented by this "ring-like" monitor structure > The image contrast is not enough, so a ring-like resist pattern cannot be printed. Turning to the system shown in Figure 4 (c), the 0HR monitor 10 presents a symmetrical phase spectrum within the limit of soil να, and all phases The range is from 0 to 36 °. When comparing the two at the printing threshold of 0.3 to 0.35 intensities, the 0hr monitor-21-I paper scale is suitable for wealth _ home scale (⑽) A4 size (21GX297 public love) -------- 1239434
视器1 0的空間影傻 〜像(如圖4(f)所示)與該Dirksen監視器所產 生之空間影像(如圖4fH、糾—、扣门 ^ , 卜 、 口 4(d)所不)相同。然而,雖然並不明顯 a ^ ^界強度大小處’内及外空間影像的對數斜率比OHR 现視⑽、、、口構1 0更為平衡。此係藉由圖4⑷及圖4⑴中的一 對箭號所示。 圖5(a) 5(c)所tf的係圖3 (a)所示之〇1^透鏡監視器結構 〇之實際印刷效㈣。用於產生圖5 (a) 5⑷之印刷情況係與 圖1(a)-1(f)所述之情況相同。圖5(a)所示的係當投影在該 投影透鏡時(I表示強度)之〇HR監視器結構1〇之二維空間影 像。圖5(b)所示的係與〇HR監視器結構(換言之該〇HR監視 器結構係由該印刷製程所產生)重疊之原始抗蝕圖案(換言之 特徵12)之俯視圖。如圖5(a)-5(c)所示,即使非常微小之 彗形像差都可以被監視器丨〇偵測到。 更特別的是,在圖5(a)及圖5(b)之2-D空間影像中可以觀 測到該模擬中已經加入彗形像差(Z7及Z 8皆為0.025又)。參 考圖5 (b),該像差係藉由將該印刷〇HR結構之内環丨4往右 上方偏移。最後,圖5 (c),其係該印刷〇HR結構之剖面圖 ,所示的係(該剖面圖的)該印刷OHR結構左側的内部} 6往 中間移動的程度大於該印刷OHR結構右側之内部1 7往中間 移動的程度。每一上述之OHR結構之位置的偏移/變化都表 示透鏡像差之存在。在沒有透鏡像差的情況下,圖5(b)之 内環1 4與用以形成該OHR監視器結構1 〇之每一正方形特徵 1 2的間隔相同。此外,圖5 ( c)之抗蝕圖案1 6,1 7與中心點 的間隔相同。 -22- 本紙張尺度適用中國國家標準(CNS) A4规格(21〇x 297公爱) 1239434 A7 — ______ B7 7、發明説明(20 )~ - 一 在使用時要注意的是,該〇HR監視器,其係印刷在刻劃線 (scribe line)内或在晶粒内以免干預到電路運作,可以被測 量以監視在對應的曝光範圍中之實際透鏡像差。接著會利 用透鏡像差以計算將C D失誤降至最小所需之必要的校正動 作舉例未說,可以藉由改變光罩圖案或調整曝光工具以 完成校正動作。如此處所說明的,透鏡像差總量可以藉由 測量該相對環寬度或相對於不受透鏡像差影響之已知的參 考結構之内環之相對偏移位置來決定。另外一種可能之方 法係藉由拍攝該印刷0Hr圖案之SEM照片並且將其與具有 已知透鏡像差之OHR圖案系列進行比對。利用統計分析, 可以重複地決定透鏡像差之大小及型式。 有關於本發明之OHR監視器的一項重點係該監視器的效能 不會因為有缺陷的光罩製程而降低。更特別的是,如果該 石英蚀刻在光罩上造成傾斜相位邊緣的話,該〇Hr監視器 並不會喪失透鏡像差偵測的敏感度。圖6(a)所示的係形成 於違光罩中(S表示光罩基板)之〇HR監視器結構丨〇之上方及 剖面圖,其中該光罩形成過程會產生具有傾斜邊之正方形 特徵12。該傾斜邊係由於在形成光罩期間使用具有缺陷之 石英上邊緣製程所造成的結果。然而,參考圖6(b),已知 該光罩上的傾斜石英相位邊緣圖案並不會對該物件相位光 磺產生重大的影響。該所有的物件光譜相位只會被些微地 壓縮(至大約為350度)。此類壓縮會使得該透鏡像差偵測監 視器之敏感度些許的下降。然而,更重要的是,即使對極 端的傾斜相位邊而言,如圖6 (c) - 6 (e)所示,亦只會對該印 -23- 1239434 A7 ——;_________ B7 五、發明説明(21 ) 刷抗蚀形狀產生極少的影響。因此,與Dirksen監視器相比 ’本發明之OHR監視器提供一種更多功能的監視器。要注 意的是用以產生圖6 ( c) - 6 (e)之印刷情況係與上面圖1 ( a) -1 ( f)所述的情況相同。 如先前所說明的,希望利用本發明之透鏡像差監視器在生 產印刷過程中進行現場監視。為了完成此目的,必須滿足 下列的條件: (1) 該透鏡像差監視器必須利用相同的光罩製程製造,不 需要額外的處理步驟;以及 (2) 當在與生產圖案之印刷相同的曝光情況下進行印刷時 該透鏡像差監視器結構必須能夠使用並且有效。 本發明之OHR監視器能夠滿足此兩項條件。圖7(a)-7(d) 證明本發明之OHR監視器可以利用於6% attPSM或雙黃光罩 中。要注意的是用於產生圖7(a)-7(d)之印刷情況係與上述 圖1 ( a ) -1 ( f)的情況相同。 更特別的是,圖7 ( a)所示的係該抗蝕圖案之俯視圖,其 係在6% attPSM中形成的,與所產生的印刷〇HR監視器結構 重疊。圖7(b)係由圖7(a)之抗蚀圖案所產生之印刷〇hr監 視器結構之剖面圖。圖7 (c)所示的係該抗蝕圖案之俯視圖 ,其係在雙黃光罩中形成的,與所產生的印刷OHR監視器 結構重疊。圖7(d)係由圖7(c)之抗蚀圖案所產生之〇hr監 視器結構之剖面圖。 從圖7(a)-7 (d)中可以清楚得知,利用6% attPSM形成之 OHR監視器結構及利用雙黃光罩形成之〇HR監視器結構兩 -24- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 1239434 A7 B7The space shadow of the viewer 10 (as shown in Figure 4 (f)) and the space image generated by the Dirksen monitor (see Figure 4fH, correction—, door ^, bu, mouth 4 (d)) Not the same. However, although it is not obvious that the logarithmic slopes of the inner and outer space images at the intensity level of the a ^^^ are more balanced than OHR's current view, 、, and 构 10. This is shown by a pair of arrows in Figure 4⑷ and Figure 4⑴. The tf shown in Figs. 5 (a) and 5 (c) is the actual printing effect of the lens monitor structure 〇 shown in Fig. 3 (a). The printing conditions used to produce Figures 5 (a) and 5⑷ are the same as those described in Figures 1 (a) -1 (f). Fig. 5 (a) is a two-dimensional spatial image of the HR monitor structure 10 when projected on the projection lens (I represents intensity). FIG. 5 (b) is a plan view of the original resist pattern (in other words, feature 12) that overlaps with the HR monitor structure (in other words, the HR monitor structure is generated by the printing process). As shown in Figures 5 (a) -5 (c), even very small coma aberrations can be detected by the monitor. More specifically, in the 2-D space image of Fig. 5 (a) and Fig. 5 (b), it can be observed that coma aberration has been added to the simulation (both Z7 and Z 8 are 0.025 again). Referring to FIG. 5 (b), the aberration is shifted to the upper right by the inner ring 4 of the printed HR structure. Finally, FIG. 5 (c) is a cross-sectional view of the printed OHR structure, which shows (in the cross-sectional view) the inner portion of the left side of the printed OHR structure. The extent to which the interior 17 moves towards the middle. The shift / change in the position of each of the above-mentioned OHR structures indicates the existence of lens aberrations. In the absence of lens aberrations, the inner ring 14 of Fig. 5 (b) has the same interval as each square feature 12 used to form the OHR monitor structure 10. In addition, the intervals between the resist patterns 16 and 17 in FIG. 5 (c) and the center point are the same. -22- This paper size is in accordance with Chinese National Standard (CNS) A4 specification (21〇x 297 public love) 1239434 A7 — ______ B7 7. Description of the invention (20) ~-When using it, please note that the HR monitoring The device is printed in a scribe line or in a die to prevent interference with circuit operation, and can be measured to monitor actual lens aberrations in the corresponding exposure range. Next, lens aberrations will be used to calculate the necessary corrective actions required to minimize CD errors. Examples are not mentioned. The corrective action can be accomplished by changing the mask pattern or adjusting the exposure tool. As explained herein, the total amount of lens aberration can be determined by measuring the relative ring width or the relative offset position of the inner ring relative to a known reference structure that is not affected by lens aberrations. Another possible method is to take a SEM picture of the printed 0Hr pattern and compare it with a series of OHR patterns with known lens aberrations. Using statistical analysis, the size and type of lens aberration can be repeatedly determined. An important point about the OHR monitor of the present invention is that the performance of the monitor will not be reduced due to a defective photomask process. More specifically, if the quartz etching causes oblique phase edges on the reticle, the OHr monitor does not lose the sensitivity of lens aberration detection. The system shown in FIG. 6 (a) is formed above and a cross-sectional view of the HR monitor structure, which is formed in the illuminating mask (S represents the reticle substrate), and the reticle forming process will produce a square feature with inclined sides 12. This beveled edge is a result of the use of a defective quartz upper edge process during the mask formation. However, referring to FIG. 6 (b), it is known that the oblique quartz phase edge pattern on the reticle does not significantly affect the phase light of the object. The spectral phase of all objects is only slightly compressed (to about 350 degrees). This type of compression will slightly reduce the sensitivity of the lens aberration detection monitor. However, more importantly, even for extreme oblique phase edges, as shown in Figures 6 (c)-6 (e), only the seal -23-1239434 A7 ——; _________ B7 V. Invention Note (21) The shape of the brush resist has little effect. Therefore, the OHR monitor of the present invention provides a more versatile monitor than a Dirksen monitor. It should be noted that the printing conditions used to produce Figures 6 (c)-6 (e) are the same as those described in Figures 1 (a) -1 (f) above. As previously explained, it is desirable to use the lens aberration monitor of the present invention for on-site monitoring during production printing. In order to accomplish this, the following conditions must be met: (1) the lens aberration monitor must be manufactured using the same mask process without the need for additional processing steps; and (2) when exposed to the same exposure as the printed pattern The lens aberration monitor structure must be usable and effective when printing is performed. The OHR monitor of the present invention can satisfy both of these conditions. Figures 7 (a) -7 (d) prove that the OHR monitor of the present invention can be used in a 6% attPSM or double yellow mask. It should be noted that the printing conditions used to produce Figs. 7 (a) -7 (d) are the same as those in Figs. 1 (a) -1 (f) described above. More specifically, the top view of the resist pattern shown in Fig. 7 (a) is formed in a 6% attPSM and overlaps with the generated printed HR monitor structure. Fig. 7 (b) is a cross-sectional view of a printed 0hr monitor structure produced by the resist pattern of Fig. 7 (a). The top view of the resist pattern shown in FIG. 7 (c) is formed in a double yellow mask and overlaps with the structure of the printed OHR monitor produced. Fig. 7 (d) is a cross-sectional view of a 0hr monitor structure generated from the resist pattern of Fig. 7 (c). It can be clearly seen from Figures 7 (a) -7 (d) that the OHR monitor structure formed by 6% attPSM and the HR monitor structure formed by double yellow masks are used. -24- This paper is applicable to China Standard (CNS) A4 (210 X 297 mm) 1239434 A7 B7
五、發明説明 者皆可以偵測到細微的透鏡像差(例如〇.025 λ )。舉例來說 ,圖7(a)及7(c)所產生的OHR監視器結構之内環14係往右 上方之方向偏移’與圖5(b)所示之〇HR監視器結構的方式 相同,從而可以有效地偵測到在該模擬所加入的〇 〇25入透 鏡像差。 要注思的疋為了確保在相關的產品圖案會使用相同的曝光 準位,對6% attPSM及雙黃光罩應用來說都必須將該〇HRi 方形12之尺寸重新調整成《〇·35(入/ΝΑ)。其它的0HR設計 參數則沒有改變。然而,因為使用較大的正方形元件,其 證明必須重新調整每一正方形元件之間的間隔以達到最佳 的網版效果。 如上所說明的,本發明之OHR監視器具有非常多功能。舉 例來說,除了偵測彗形像差以外,連同上面的圖5,6及7所 示’該OHR監視器也可以偵測各種類型的透鏡像差。圖 8(a)-8(h)所示的係〇HR監視器偵測透鏡像差之能力。要注 意的是用於生產圖8(a)-8(h)之印刷狀況係與上面圖1(a)_ 1 (f)所述之情況相同,除了該透鏡像差設定以外,所有都 具有+ 0.1 μηι的失焦。 圖8(a)所示的係用於形成該〇HR監視器結構並且利用繞 射限制透鏡印刷所產生之〇HR監視器結構重疊之抗蝕圖案 之俯視圖。圖8(e)所示的係符合圖8(a)之OHR監視器之投 影透鏡瞳孔處之波前。如圖所示,當内環丨4及外環丨5皆在 預期的位置時,該印刷〇HR監視器結構會指示該透鏡實質 上係無像差。 -25- 本紙張尺飘财_家標準(CNS) M規格(2iqχ撕公董) 1239434 A7Fifth, the invention can detect subtle lens aberrations (for example, 0.025 λ). For example, the inner ring 14 of the OHR monitor structure produced in Figs. 7 (a) and 7 (c) is shifted to the upper right direction and the way of the HR monitor structure shown in Fig. 5 (b). The same, so that it can effectively detect the 0.25 lens aberration added in the simulation. It is important to note that in order to ensure that the same exposure level will be used in related product patterns, for 6% attPSM and double yellow mask applications, the size of the 0HRi square 12 must be readjusted to "〇 · 35 ( Into / ΝΑ). Other 0HR design parameters remain unchanged. However, because larger square elements are used, it proves that the spacing between each square element must be readjusted to achieve the best screen effect. As explained above, the OHR monitor of the present invention is very versatile. For example, in addition to detecting coma aberrations, the OHR monitor can also detect various types of lens aberrations, as shown in Figures 5, 6, and 7 above. The ability of the HR monitor to detect lens aberrations shown in Figures 8 (a) -8 (h). It should be noted that the printing conditions used to produce Figures 8 (a) -8 (h) are the same as those described in Figures 1 (a) -1 (f) above, except for the lens aberration setting, all of which have + 0.1 μηι out of focus. FIG. 8 (a) is a plan view of a resist pattern for forming the HR monitor structure and overlapping the HR monitor structure produced by printing with a diffraction-limiting lens. The wavefront at the pupil of the projection lens of the OHR monitor shown in Fig. 8 (e) is shown in Fig. 8 (e). As shown in the figure, when the inner ring 4 and the outer ring 5 are in the expected positions, the printed HR monitor structure will indicate that the lens is essentially aberration-free. -25- This paper ruler is floating _home standard (CNS) M size (2iqχ tear public director) 1239434 A7
圖8(b)所示的係印刷時具有45度散光之〇〇5λ透鏡像差之 透鏡像差監視器結構之抗蝕圖案之俯视圖。圖8(f)所示的 係符合圖8(b)之OHR監视器結構之投影透鏡瞳孔處之波前 。如圖所示,該OHR監視器結構可以藉由沿著以度軸延長 内環1 4以顯示出該透鏡像差。 圖8 ( c)所示的係印刷時具有χ及γ彗形(27及28) 〇 〇5入透 鏡像差之透鏡像差監視器結構之抗蝕圖案之俯視圖,與所 產生的OHR監視器結構重疊。圖8(g)所示的係符合圖8(幻 之OHR監視器結構之投影透鏡瞳孔處之波前。如圖所示, 該印刷OHR監視器結構藉由將内環丨4及外環丨5往向上及往 右偏移以顯示該透鏡像差。 圖8(d)所示的係印刷時具有X及γ傾斜(Z2及23) 〇 〇5又 透鏡像差之透鏡像差監視器結構之抗蝕圖案之俯視圖,與 所產生的OHR監視器結構重疊。圖8 (h)所示的係符合圖 8(d)之OHR監視器結構之投影透鏡瞳孔處之波前。如圖所 示’該印刷OHR監視器結構藉由將内環丨4及外環丨5往向下 及往左偏移以顯示該透鏡像差。 因此,即使實際的透鏡像差可能非常複雜及細小,結合本 發明之OHR監視器及最新的度量衡工具,便可以分析透鏡 像差之潛在原因。要注意的是當觀視投影在圖之 投影透鏡瞳孔處的波前時,也可以明顯地看見圖8(a)_8(h) 所辨識之透鏡像差。 圖9所示的係適用於本發明之微影投影裝置示意圖。該裝 置包括: -26-本紙張尺度適用中國國家標準(CNS) A4規格(21〇χ 297公釐) 1239434Fig. 8 (b) is a plan view of a resist pattern of a lens aberration monitor structure having a 005λ lens aberration of 45 degrees astigmatism at the time of printing. The wavefront at the pupil of the projection lens conforming to the structure of the OHR monitor shown in Fig. 8 (b) is shown in Fig. 8 (f). As shown, the OHR monitor structure can show the lens aberration by extending the inner ring 14 along the axis of degrees. Figure 8 (c) shows the top view of the resist pattern of the lens aberration monitor structure with χ and γ coma (27 and 28) at the time of printing, and the resulting OHR monitor Structures overlap. The system shown in Fig. 8 (g) corresponds to the wavefront at the pupil of the projection lens of Fig. 8 (Magic OHR monitor structure. As shown in the figure, the printed OHR monitor structure consists of the inner ring 4 and the outer ring 丨5 is shifted up and to the right to display the lens aberration. The system shown in Figure 8 (d) has X and γ tilts (Z2 and 23) when printing, and a lens aberration monitor structure with lens aberration. The top view of the resist pattern overlaps with the produced OHR monitor structure. Figure 8 (h) shows the wavefront at the pupil of the projection lens that conforms to the OHR monitor structure of Figure 8 (d). As shown in the figure 'The printed OHR monitor structure displays the lens aberration by shifting the inner ring 4 and the outer ring 5 down and to the left. Therefore, even the actual lens aberration may be very complicated and small. The invented OHR monitor and the latest metrology tools can analyze the potential causes of lens aberrations. It should be noted that when viewing the wavefront projected on the pupil of the projection lens of the figure, you can also clearly see Figure 8 (a ) _8 (h) The aberration of the lens identified. Figure 9 is a schematic illustration of a lithographic projection device suitable for the present invention. The apparatus comprises: -26- This paper scales applicable Chinese National Standard (CNS) A4 size (297 mm 21〇χ) 1239434
照射系統Ex,IL,用以提供照射(例如UV或EUV照射 )<投影光束PB。在此特殊例子中,該照射系統也包括一種 照射源LA ; • 一第一物件平台(光罩平台)MT配備一承托光罩MA(例如 標線)之光罩承托器,並且連接至該第一定位構件用以準確 地相對該P L定位該光罩; 一第二物件平台(基板平台)WT配備一承托基板w(例如 塗佈抗敍之矽晶圓)之基板承托器,並且連接至該第二定位 構件用以準確地相對該PL定位該基板; •一投影系統(”透鏡,,)PL(例如折射,全折光或反射光學 陣列)用以將該光罩MA之照射位置映射在該基板界之目標部 分C (例如包括一個或多個晶粒)。 如此處所述,該設備係一種傳導類型(換言之具有一傳導光 罩)。然而,一般來說,其也係為一種反射類型,舉例來說( 具有一反射光罩)。例外,該設備可以使用另一種圖案構件 ,例如上述的可程式鏡陣列。 光源LA(例如水銀燈(Hg Lamp),準分子雷射,或離子光 源)會產生照射光束。此光束會送入照度系統(照明器)IL中 ’直接送入或是穿越過調整構件之後再送入,例如光束擴 張器Ex。該照明器IL包括用以設定該光束強度分配之外圈 以及/或是内圈範圍(通常分別稱之為σ -外部及σ -内部)的 調整構件AM。此外,其通常包括各種其它的要件,例如整 合器IN以及聚光器C 0。依照此方法,光束p b會照射在光罩 Μ A上於其橫切面上具有所希望之均句性及強度分配。 -27- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 1239434 A7 B7 五、發明説明(25 ) 接著光束PB會碰觸支撐在光罩平台MT上之光罩MA。穿 越過光罩MA後,光束PB會通過透鏡PL,其將光束PB聚焦 至基板W之目標部分C。利用該第二定位構件(以及干涉計 測量構件IF ),可以準確地移動該基板平台WT,因而可以 定位在光束PB路徑中不同的目標部分C。同樣地,在從光 罩庫中以機械方式取出光罩MA,或是在掃描期間,該第一 定位構件可以準確定位在光束PB路徑中之光罩μα。一般 來說,物件平台MT的移動,WT會利用長擊(long-str〇ke) 模組(粗定位(coarse positioning))以及短擊模組(short-stroke) ( 細定位 (fine positioning)) , 圖 9 中並未 明確地 顯示。 然而,至於晶圓步進器(與步進掃描裝置相反),該光罩平台 MT可能會連接至短擊啟動器,或可能固定不動。 該描述裝置可以使用在兩種不同模式: -在步進模式中,該光罩平台MT基本上係保持不動,而 整個光罩影像則係一次(換言之一次”閃光”)整個投影至目 標部分C。接著該基板平台WT會在X以及/或是y方向移動 使得該光束PB可以照射不同的目標部分c ; -在掃描模式中,基本上是相同的情況,除了已知目標部 分C並不是以一次”閃光,,進行曝光之外。取代的是,該光罩 平台MT可以以速度u在已知的方向(所謂的”掃描方向,,, 例如y万向)移動,使得該投影光束pB可以在光罩影像上掃 描j同時,該基板平台wt係同時以速度v = Mv在相同或相 反方向私動,其中M係透鏡PL之放大倍率(通常,1/4或 )移動。依照此方式,可以曝光較大的目標部分c,但是 -28-The irradiation system Ex, IL is used to provide irradiation (e.g. UV or EUV irradiation) < projected light beam PB. In this particular example, the illumination system also includes an illumination source LA; • a first object platform (mask platform) MT is equipped with a mask holder that supports a mask MA (eg, a marking line), and is connected to The first positioning member is used to accurately position the photomask relative to the PL; a second object platform (substrate platform) WT is provided with a substrate holder that supports a substrate w (such as a coated silicon wafer), And is connected to the second positioning member to accurately position the substrate relative to the PL; a projection system ("lens,") PL (such as a refractive, full-refractive or reflective optical array) is used to illuminate the mask MA The position is mapped to a target portion C of the substrate boundary (for example, including one or more dies). As described herein, the device is a conductive type (in other words, it has a conductive mask). However, in general, it is also a Is a type of reflection, for example (with a reflective mask). Exceptionally, the device can use another patterned component, such as the programmable mirror array described above. Light source LA (eg mercury lamp, excimer laser) (Or ion light source) will generate an illumination beam. This beam will be sent to the illumination system (illuminator) IL 'directly or after passing through the adjustment member, such as the beam expander Ex. The illuminator IL includes for setting The beam intensity is assigned to the adjusting member AM of the outer and / or inner ring ranges (commonly referred to as σ-outer and σ-inner, respectively). In addition, it usually includes various other elements, such as an integrator IN and a condenser Device C 0. According to this method, the light beam pb will be irradiated on the photomask M A with the desired uniformity and intensity distribution on its cross-section. -27- This paper size applies the Chinese National Standard (CNS) A4 specification 210 X 297 mm) 1239434 A7 B7 V. Description of the invention (25) Then the beam PB will touch the mask MA supported on the mask platform MT. After passing through the mask MA, the beam PB will pass through the lens PL, which will The light beam PB is focused to the target portion C of the substrate W. With the second positioning member (and the interferometer measurement member IF), the substrate platform WT can be accurately moved, and thus different target portions C in the path of the light beam PB can be positioned. Ground, when the mask MA is mechanically taken out from the mask library, or during scanning, the first positioning member can accurately position the mask μα in the path of the beam PB. Generally speaking, the movement of the object platform MT, WT uses long-stroke modules (coarse positioning) and short-stroke modules (fine positioning), which are not explicitly shown in Figure 9. However, as for the wafer stepper (as opposed to a step-and-scan device), the reticle platform MT may be connected to a short-stroke starter, or it may be fixed. The description device can be used in two different modes:-In the step mode, the mask platform MT is basically kept stationary, and the entire mask image is projected once (in other words, "flash") to the entire target portion C . Then the substrate platform WT will move in the X and / or y direction so that the light beam PB can illuminate different target portions c;-in the scanning mode, it is basically the same situation, except that the target portion C is not known once. Instead of exposure, the mask platform MT can be moved at a speed u in a known direction (the so-called “scanning direction,” for example, y-universal), so that the projection beam pB can be at At the same time as scanning j on the mask image, the substrate platform wt moves at the same time in the same or opposite direction at a speed v = Mv, where the magnification of the M lens PL (usually, 1/4 or) moves. In this way, a larger target portion c can be exposed, but -28-
1239434 A7 B7 五、發明説明(26 ) 卻不會影響解析度。 本發明可以,舉例來說,可用於檢查在照明器IL以及/或 是上述裝置之投影系統PL中的像差。 如上所提,可以對本發明之OHR監視器之示範具體實例進 行各種變化。舉例來說,雖然示範之OHR監視器結構係環 形形狀,無疑地也可以是其它的形狀。此外,用於形成 OHR監視器結構之個別特徵也可以不是正方形。 此外,該OHR可以用於所有類型之光罩中,舉例來說,雙 黃,attPSM,交替式PSM,以及無色PSM。因為該OHR設計 指示此類結構及特徵間隔對透鏡像差非常敏感,所以該 OHR的設計尺寸可以作為積體電路設計中”禁止 (forbidden)”之設計規則參考。因此,該電路特徵會變得比 較不會受透鏡像差之影響。此對記億電路或資料庫電路設 計非常重要,可以強化/改善CD控制。 如上所述,本發明之OHR監視器提供優於該先前技藝之重 要優點。更重要的係,本發明提供一種透鏡監視器可以偵 測到非常細微的透鏡像差,其不會受到用於形成該監視器 之光罩形成過程中之缺陷的影響。 此外,本發明之透鏡像差監視器適用於現場監視,因為該 透鏡監視器可以利用形成生產光罩所需之相同光罩形成過 程來形成,因此不需要額外的光罩形成程序步驟。此外, 因為該透鏡監視器結構之全部尺寸非常小,所以該結構可 以放置在許多位置以監視整個曝光範圍。 還有另一項優點係,因為本發明之透鏡像差監視器結構利 -29- 本紙張尺度適用中國國家標準(CNS) A4規格(210 X 297公釐) 1239434 A7 B7 五、發明説明(27 ) 用次解晰特徵,該特徵之實際形狀以及尺寸不是非常重要 ,因此該透鏡像差監視器在實際應用中偵測像差的效果非 常的好。 最後’也要注意的是雖然在前面的說明中可以參考積體電 路製造中的微影投影裝置,不過應該明白此類裝置具有其 它的應用。舉例來說,其可以用於積體光學系統之製造, 磁性記憶體之導引及偵測圖案,液晶顯示器面板(panel), 薄膜磁頭等。熟習本技藝之人士將會了解,在此替代應用 之内容中,可以將本文中所用到的專有名詞”標線"或"晶圓 ’’以更普遍之專有名詞,,光罩”或,,基板”取代。 在本文案中,專有名詞”照射”及”光束”係用以涵蓋所有 類型的電磁照射,包括紫外線照射(例如波長365,248, 193,157或126nm)及EUV(極度紫外線照射,例如波長範圍 為 5 -20nm)。 雖然已揭露本發明之某些特定具體實例,要注意的是本發 明可以在不達反本發明精神或本質特徵之情況下以其它特 足型式具體化。因此,本發明在各方面僅係解釋而非限制 ’本發明範圍係由隨附之申請專利範圍所表示而非前面的 敘述’因此所有符合申請專利範圍之等效範圍中的意義都 涵蓋於其中。 30- 本紙張尺度適用巾® ®家標準(CNS) A4規格(21G X 297公董)1239434 A7 B7 5. The invention description (26) does not affect the resolution. The invention can, for example, be used to check aberrations in the illuminator IL and / or the projection system PL of the above-mentioned device. As mentioned above, various changes can be made to the exemplary embodiment of the OHR monitor of the present invention. For example, although the exemplary OHR monitor structure has a circular shape, it is no doubt that other shapes are also possible. In addition, the individual features used to form the OHR monitor structure may not be square. In addition, the OHR can be used in all types of reticle, for example, double yellow, attPSM, alternating PSM, and colorless PSM. Because the OHR design indicates that such structures and feature intervals are very sensitive to lens aberrations, the design size of the OHR can be used as a reference for "forbidden" design rules in integrated circuit design. As a result, the circuit characteristics become less affected by lens aberrations. This is very important for the design of the Billion Circuit or Library Circuit, which can strengthen / improve the CD control. As mentioned above, the OHR monitor of the present invention provides important advantages over this prior art. More importantly, the present invention provides a lens monitor capable of detecting very fine lens aberrations, which is not affected by defects in the process of forming a mask for forming the monitor. In addition, the lens aberration monitor of the present invention is suitable for on-site monitoring because the lens monitor can be formed using the same mask formation process required to form a production mask, and therefore no additional mask formation process steps are required. In addition, because the overall size of the lens monitor structure is very small, the structure can be placed in many positions to monitor the entire exposure range. There is another advantage because the structure of the lens aberration monitor of the present invention is advantageous. 29- This paper size is applicable to China National Standard (CNS) A4 (210 X 297 mm) 1239434 A7 B7 V. Description of the invention (27 ) Use the sub-resolution feature. The actual shape and size of the feature are not very important, so the lens aberration monitor has a very good effect in detecting aberrations in practical applications. Finally, it should also be noted that although the lithographic projection device in the manufacture of integrated circuits can be referred to in the previous description, it should be understood that such devices have other applications. For example, it can be used in the manufacture of integrated optical systems, magnetic memory guidance and detection patterns, liquid crystal display panels, thin film magnetic heads, and the like. Those skilled in the art will understand that in the content of this alternative application, the proper nouns used in this article, "marking lines" or "wafers", can be more commonly used, and masks "Or, substrate" instead. In this case, the proper terms "irradiation" and "beam" are used to cover all types of electromagnetic radiation, including ultraviolet radiation (such as wavelengths 365, 248, 193, 157 or 126nm) and EUV (extreme ultraviolet radiation, for example, a wavelength range of 5-20 nm). Although certain specific examples of the present invention have been disclosed, it should be noted that the present invention can be used for other special features without departing from the spirit or essential characteristics of the present invention. The foot type is specific. Therefore, the present invention is merely an explanation and not a limitation in all aspects. The scope of the present invention is indicated by the scope of the appended patent application rather than the foregoing description. Significance is included in it. 30- This paper size applies Towel ® ® Home Standard (CNS) A4 specification (21G X 297)
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JP3910065B2 (en) | 2007-04-25 |
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